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M. Lei et al. / Journal of Alloys and Compounds 639 (2015) 102–105
Fig. 4. Room temperature PL spectra of BaMoO4 obtained at the following typical
experimental concentrations (a) 1.0 mL/L PSMA, 0.5 mM BaCl2 and 0.5 mM
Na2MoO4 (b) 2.0 mL/L PSMA, 0.7 mM BaCl2 and 0.7 mM Na2MoO4, (c) 0.25 mL/L
PSMA, 0.3 mM BaCl2 and 0.3 mM Na2MoO4.
reduced while their volumes increased as the PSMA/Ba2+ ratio
increases. This may occur because of the well-known Ostwald
Ripening process [49] that the small crystals dissolve first and then
redeposit onto larger crystals to maintain the minimum system
energy. When the local PSMA concentration is high but not enough
to completely inhibit the crystallization of BaMoO4, large particles
usually have lower energy and thus more stable than the small
particles, promoting the Ostwald Ripening process.
Fig. 3. Schematic formation mechanisms of BaMoO4 crystals at different concen-
trations of both PSMA and reactants.
usually have different surface energies, and it is known that crystal
plane with high surface energy grows faster than those with lower
surface energy. PSMA will selectively adsorb on the high-surface-
energy plane, decreasing the local Ba2+ concentration by forming
new PSMA–Ba chain, and inhibiting crystal growth in this direction
by lowering the surface energy. When PSMA is sufficient, the
inhibition in the initially dominant growth directions will be
obvious, causing the morphology of ellipsoid. On the contrary, an
increase in reactants concentration will weaken such inhibition,
explaining the morphology evolution from ellipsoid to elongated
octahedron in group C. These results agree with the analysis of
Yu et al. in that the morphology of crystal is determined by the
adsorptive feature of different PSMA concentration [48]. In
addition, when the local PSMA concentration is much higher than
the Ba2+ concentration, the strong PSMA–Ba complexion will inten-
sively decline the combination of Ba2+ and MoO42À, leading to the
incomplete or irregular crystal morphology (sample A1 and B1).
Fig. 3b shows the schematic evolution mechanisms of the
octahedron or spindle-like to flower-like crystal at moderate or
high PSMA concentration. This transformation process could also
be ascribed to the inhibition of PSMA. Unlike low PSMA concentra-
tion, as PSMA/Ba2+ ratio increases, the surface energy of those
original preferential-growth crystal planes will lower to an extent
that almost identical to that of other crystal planes, thus the crystal
will not only grow along the long axis, but also have the potential
to grow along other direction, achieving the transformation from
one-dimensional growth to multi-dimensional growth. When the
PSMA/Ba2+ ratio is low, the samples will exhibit distinct crystalline
characteristics at different absolute PSMA concentration. At mod-
erate PSMA concentration (Fig. 3b, left), two kinds of crystal mor-
phologies could coexist. It appears that part of the octahedral
nuclei will form the flower-like crystals whereas the remaining
nuclei will grow into big octahedrons. Conversely, local high
PSMA will modulate the growth of nuclei directly, forming the
spindle-like nuclei (Fig. 3b, right). This may explain the sharpness
of the crystal edge and the morphology evolution at two different
PSMA concentrations. It is also found that the number of particles
The optical properties of BaMoO4 nanocrystals were investi-
gated by the photoluminescence (PL) technique. Fig. 4 illustrates
the PL spectra of the typical BaMoO4 samples with excitation
wavelength of 325 nm at room temperature. The samples exhibit
broad green emission peaks of 530 nm, which is consistent with
previous data [26,50,51]. It is well accepted that the emission spec-
tra of metal molybdates are mainly caused by the electronic charge
transfer within the MoO24À unit [27,52]. Previous reports [53,54]
analyze the PL spectra of compounds by the Peakfit deconvolution
program. Based on this method, the PL spectra of BaMoO4 can be
deconvolved into several Gaussian peaks. Using Sample A as an
example, we can get five component curves at 410 nm (8%),
445 nm (13%), 493 nm (16%), 525 nm (48%) and 595 nm (15%),
which represents different types of electronic transitions and
specific atomic arrangements. Abreu et al. [54] attribute the
blue–green emission to an ordered structure with shallow defects,
while the yellow–orange–red emission is caused by a disordered
structure with deep defects. According to the principle of MoO42À
complexes, the coupling between the O-2p (r) and O-2p (p) orbi-
tals and Mo-4d (t2) and Mo4d (e) orbitals are responsible for the
hybridization of molecular orbitals. Among those electron states,
only the 1T2 ? 1A1 transition is allowed [27,55]. We ascribe the
blue and green emission to 1T2 ? 1A1 transition in the intrinsic
MoO24À group (shallow defects) and the orange emission to the
defect MoO3 group (deep defects) [56]. The additional emissions
can be explained by the Jahn–Teller splitting effect [31]. In particu-
lar, our previous study on the photoluminescence of BaMoO4
shows intense blue emission and weak green emission at the same
wavelengths [56], we conjecture this may induced by differences
in the crystal structures. However, accurate explanation for the
PL spectra of BaMoO4 remains to be further explored. There are
many factors that govern the photoluminescence properties of
BaMoO4, such as particle size, crystalline degree, morphology,
and surface defects [55,56]. As is shown in Fig. 4, homogeneous
distribution and small particle size are important factors to
enhance the PL intensity, for crystals with such morphology usu-
ally have fewer dead layers [31,47].